• Luigi Pacciani
  • Dawoon E. Kim
  • Riccardo Middei
  • Herman L. Marshall
  • Alan P. Marscher
  • Ioannis Liodakis
  • Iván Agudo
  • Juri Poutanen
  • Manel Errando
  • Laura Di Gesu
  • Michela Negro
  • Fabrizio Tavecchio
  • Kinwah Wu
  • Chien-Ting Chen
  • Fabio Muleri
  • Lucio Angelo Antonelli
  • Immacolata Donnarumma
  • Steven R. Ehlert
  • Francesco Massaro
  • Stephen L. O'Dell
  • Matteo Perri
  • Simonetta Puccetti
  • Francisco José Aceituno
  • Giacomo Bonnoli
  • Víctor Casanova
  • Juan Escudero
  • Beatriz Agís-González
  • César Husillos
  • Daniel Morcuende
  • Jorge Otero-Santos
  • Alfredo Sota
  • Pouya M. Kouch
  • Elina Lindfors
  • George A. Borman
  • José L. Gómez
  • Evgenia N. Kopatskaya
  • Alexey V. Zhovtan
  • Dmitry Blinov
  • Anastasia Gourni
  • Sebastian Kiehlmann
  • Angelos Kourtidis
  • Nikos Mandarakas
  • Efthymios Palaiologou
  • Nikolaos Triantafyllou
  • Anna Vervelaki
  • Ioannis Myserlis
  • Mark Gurwell
  • Garrett Keating
  • Ramprasad Rao
  • Emmanouil Angelakis
  • Alexander Kraus
  • Matteo Bachetti
  • Luca Baldini
  • Wayne H. Baumgartner
  • Ronaldo Bellazzini
  • Stefano Bianchi
  • Stephen D. Bongiorno
  • Raffaella Bonino
  • Alessandro Brez
  • Niccoló Bucciantini
  • Fiamma Capitanio
  • Simone Castellano
  • Elisabetta Cavazzuti
  • Stefano Ciprini
  • Enrico Costa
  • Alessandra De Rosa
  • Ettore Del Monte
  • Niccoló Di Lalla
  • Alessandro Di Marco
  • Victor Doroshenko
  • Michal Dovčiak
  • Teruaki Enoto
  • Yuri Evangelista
  • Sergio Fabiani
  • Riccardo Ferrazzoli
  • Javier A. Garcia
  • Shuichi Gunji
  • Kiyoshi Hayashida
  • Jeremy Heyl
  • Wataru Iwakiri
  • Philip Kaaret
  • Vladimir Karas
  • Fabian Kislat
  • Takao Kitaguchi
  • Jeffery J. Kolodziejczak
  • Henric Krawczynski
  • Fabio La Monaca
  • Luca Latronico
  • Simone Maldera
  • Alberto Manfreda
  • Frédéric Marin
  • Andrea Marinucci
  • Giorgio Matt
  • Ikuyuki Mitsuishi
  • Tsunefumi Mizuno
  • C. -Y. Ng
  • Nicola Omodei
  • Chiara Oppedisano
  • Alessandro Papitto
  • George G. Pavlov
  • Abel Lawrence Peirson
  • Melissa Pesce-Rollins
  • Pierre-Olivier Petrucci
  • Maura Pilia
  • Andrea Possenti
  • Brian D. Ramsey
  • John Rankin
  • Ajay Ratheesh
  • Oliver J. Roberts
  • Roger W. Romani
  • Carmelo Sgró
  • Patrick Slane
  • Paolo Soffitta
  • Gloria Spandre
  • Douglas A. Swartz
  • Toru Tamagawa
  • Roberto Taverna
  • Yuzuru Tawara
  • Allyn F. Tennant
  • Nicholas E. Thomas
  • Francesco Tombesi
  • Alessio Trois
  • Sergey S. Tsygankov
  • Roberto Turolla
  • Jacco Vink
  • Martin C. Weisskopf
  • Fei Xie
  • Silvia Zane
We report the Imaging X-ray Polarimetry Explorer (IXPE) polarimetric and simultaneous multiwavelength observations of the high-energy-peaked BL Lacertae object (HBL) 1ES 1959+650, performed in 2022 October and 2023 August. In 2022 October, IXPE measured an average polarization degree ΠX = 9.4% ± 1.6% and an electric-vector position angle ψX = 53° ± 5°. The polarized X-ray emission can be decomposed into a constant component, plus a rotating component, with the rotation velocity ωEVPA = (‑117 ± 12) deg day‑1. In 2023 August, during a period of pronounced activity of the source, IXPE measured an average ΠX = 12.4% ± 0.7% and ψX = 20° ± 2°, with evidence (∼0.4% chance probability) for a rapidly rotating component with ωEVPA = 1864 ± 34 deg day‑1. These findings suggest the presence of a helical magnetic field in the jet of 1ES 1959+650 or stochastic processes governing the field in turbulent plasma. Our multiwavelength campaigns from radio to X-ray reveal variability in both polarization and flux from optical to X-rays. We interpret the results in terms of a relatively slowly varying component dominating the radio and optical emission, while rapidly variable polarized components dominate the X-ray and provide minor contribution at optical wavelengths. The radio and optical data indicate that on parsec scales the magnetic field is primarily orthogonal to the jet direction. On the contrary, X-ray measurements show a magnetic field almost aligned with the parsec jet direction. Confronting with other IXPE observations, we guess that the magnetic field of HBLs on subparsec scale should be rather unstable, often changing its direction with respect to the Very Long Baseline Array jet.
Original languageRussian
Article number78
JournalThe Astrophysical Journal
Volume983
DOIs
StatePublished - 8 Apr 2025

ID: 134440480